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Mechanical Vibrations Forced Vibration of a Single Degree of Freedom System

Mechanical Vibrations Forced Vibration of a Single Degree of Freedom System. Philadelphia University Faculty of Engineering Mechanical Engineering Department Dr. Adnan Dawood Mohammed (Professor of Mechanical Engineering). Harmonically Excited Vibration. Physical system.

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Mechanical Vibrations Forced Vibration of a Single Degree of Freedom System

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  1. Mechanical VibrationsForced Vibration of a Single Degree of Freedom System Philadelphia University Faculty of Engineering Mechanical Engineering Department Dr. Adnan Dawood Mohammed (Professor of Mechanical Engineering)

  2. Harmonically Excited Vibration • Physical system

  3. Harmonically Excited Vibration

  4. Harmonically Excited Vibration

  5. Harmonically Excited Vibration

  6. Harmonically Excited Vibration

  7. Damped Forced Vibration System • Graphical representation for Magnification factor M and ϕ.

  8. Damped Forced Vibration System • Notes on the graphical representation of X. • For ζ = 0 , the system is reduced and becomes un-damped. • for any amount of ζ > 0 , the amplitude of vibration decreases (i.e. reduction in the magnification factor M). This is correct for any value of r. • For the case of r = 0, the magnification factor equals 1. • The amplitude of the forced vibration approaches zero when the frequency ratio ‘r’ approaches the infinity (i.e. M→0 when r → ∞)

  9. Damped Forced Vibration System • Notes on the graphical representation for ϕ. • For ζ = 0 , the phase angle is zero for 0<r<1 and 180o for r>1. • For any amount of ζ > 0 and 0<r<1, 0o<ϕ<90o. • For ζ > 0 and r>1, 90o<ϕ<180o. • For ζ > 0 and r=1, ϕ=90o. • For ζ > 0 and r>>1, ϕ approaches 180o.

  10. Harmonically Excited Vibration

  11. Harmonically Excited Vibration

  12. Forced Vibration due to Rotating Unbalance Unbalance in rotating machines is a common source of vibration excitation. If Mt is the total mass of the system, m is the eccentric mass and w is the speed of rotation, the centrifugal force due to unbalanced mass is meω2 where e is the eccentricity. • The vertical component (meω2sin(ωt) is the effective one because it is in the direction of motion of the system. The equation of motion is:

  13. Forced Vibration due to Rotating Unbalance

  14. Transmissibility of Force

  15. Transmissibility of displacement (support motion) The forcing function for the base excitation Physical system: Mathematical model:

  16. Transmissibility of displacement (support motion) Substitute the forcing function into the math. Model:

  17. Transmissibility of displacement (support motion) Graphical representation of Force or Displacement Transmissibility ((TR) and the Phase angle (f)

  18. Example 3.1: Plate Supporting a Pump: A reciprocating pump, weighing 68 kg, is mounted at the middle of a steel plate of thickness 1 cm, width 50 cm, and length 250 cm. clamped along two edges as shown in Fig. During operation of the pump, the plate is subjected to a harmonic force, F(t) = 220 cos (62.832t) N. if E=200 Gpa, Find the amplitude of vibration of the plate.

  19. Example 3.1: solution • The plate can be modeled as fixed – fixed beam has the following stiffness: • The maximum amplitude (X) is found as: -ve means that the response is out of phase with excitation

  20. Example 3.2: Find the total response of a single-degree-of-freedom system with m = 10 kg, c = 20 N-s/m, k=4000 N/m, xo = 0.01m and = 0 when an external force F(t) = Fo cos(ωt) acts on the system with Fo = 100 N and ω = 10 rad/sec . Solution a. From the given data

  21. Example 3.2: Solution • Total solution: • X(t) = X c (t) + X p(t)

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